Component of a substrate support assembly producing localized magnetic fields

- Lam Research Corporation

A component of a substrate support assembly such as a substrate support or edge ring includes a plurality of current loops incorporated in the substrate support and/or the edge ring. The current loops are laterally spaced apart and extend less than halfway around the substrate support or edge ring with each of the current loops being operable to induce a localized DC magnetic field of field strength less than 20 Gauss above a substrate supported on the substrate support during plasma processing of the substrate. When supplied with DC power, the current loops generate localized DC magnetic fields over the semiconductor substrate so as to locally affect the plasma and compensate for non-uniformity in plasma processing across the substrate.

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Description
FIELD OF THE INVENTION

Disclosed herein is a component of a substrate support assembly having a plurality of current loops adapted to generate small magnetic fields and compensate for variations during plasma processing of a semiconductor substrate supported on the substrate support assembly. The component can be an edge ring or substrate support such as a tunable electrostatic chuck (ESC) that allows for improved control of critical dimension (CD) uniformity, as well as methods and uses thereof.

BACKGROUND

In this specification where a document, act or item of knowledge is referred to or discussed, this reference or discussion is not an admission that the document, act or item of knowledge or any combination thereof was at the priority date, publicly available, known to the public, part of common general knowledge, or otherwise constitutes prior art under the applicable statutory provisions; or is known to be relevant to an attempt to solve any problem with which this specification is concerned.

Commonly-owned U.S. Pat. No. 6,921,724 discloses an etch processor for etching a wafer that includes an ESC for holding a wafer and a temperature sensor reporting a temperature of the wafer. The chuck includes a heater controlled by a temperature control system and a temperature sensor is operatively coupled to the temperature control system to maintain the temperature of the ESC at a selectable set-point temperature. A first set-point temperature and a second set-point temperature are selected. The wafer is placed on the chuck and set to the first set-point temperature. The wafer is then processed for a first period of time at the first set-point temperature and for a second period of time at the second set-point temperature.

Commonly-owned U.S. Pat. No. 6,847,014 discloses a ESC for a plasma processor comprising a temperature-controlled base, a thermal insulator, a flat support, and a heater. The temperature-controlled base has a temperature below the desired temperature of a substrate. The thermal insulator is disposed over the temperature-controlled base. The flat support holds a substrate and is disposed over the thermal insulator. A heater is embedded within the flat support and/or disposed on an underside of the flat support and includes a plurality of heating elements that heat a plurality of corresponding heating zones. The power supplied and/or temperature of each heating element is controlled independently.

Commonly-owned U.S. Patent Publication No. 2011/0092072 discloses a heating plate for a substrate support assembly in a semiconductor plasma processing apparatus comprising multiple independently controllable planar heater zones arranged in a scalable multiplexing layout, and electronics to independently control and power the planar heater zones.

Thus, there is a need for a component of a substrate support assembly, such as a substrate support assembly comprising an ESC or edge ring, which is capable of making spatial corrections and/or adjustments to the azimuthal plasma processing rate non-uniformity to correct for film thickness variation, etch chamber induced etch rate non-uniformity and large magnetic field (from plasma generation) induced non-uniformity.

While certain aspects of conventional technologies have been discussed to facilitate disclosure of the invention, Applicant in no way disclaims these technical aspects, and it is contemplated that the claimed invention may encompass or include one or more of the conventional technical aspects discussed herein.

SUMMARY

Disclosed herein is a component of a substrate support assembly comprising an edge ring or substrate support incorporating a plurality of current loops which generate small magnetic fields in a plasma during plasma processing of at least one semiconductor substrate. The component creates a localized magnetic field without the need for a permanent magnet or iron core. The magnetic fields are small enough to avoid damage to circuits undergoing processing on the semiconductor substrate but strong enough to affect the plasma so as to increase or decrease localized plasma processing such as etch rates during plasma etching. The spatial adjustments to the localized plasma processing rates can compensate for film thickness variation, chamber non-uniformity and/or magnetic field induced non-uniformity.

During plasma processing such as etching, the current loops can be powered to manipulate the plasma and effect spatial adjustments to an azimuthal plasma to correct for film thickness variation, chamber non-uniformity and/or magnetic field induced non-uniformity.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a cross-sectional view of a substrate support assembly comprising an ESC.

FIG. 2 shows a top view (FIG. 2A) of a component of a substrate support assembly in accordance with an embodiment and a cross-sectional view (FIG. 2B) of the associated perpendicular applied magnetic field. FIG. 2C shows a controller, DC power source(s), and current loop(s).

FIG. 3 shows a perspective view of a component of a substrate support assembly in accordance with an embodiment.

FIG. 4 shows a top view of a component of a substrate support assembly in accordance with another embodiment.

FIG. 5 shows a top view of a component of a substrate support assembly in accordance with yet another embodiment.

FIG. 6 shows a top view of a component of a substrate support assembly in accordance with a further embodiment.

FIG. 7 shows a top view of a component in accordance with an embodiment that surrounds a substrate support.

FIG. 8 shows a perspective view of a component in accordance with an embodiment that surrounds a substrate support.

FIG. 9 shows a top view of a component in accordance with another embodiment that surrounds a substrate support.

FIG. 10 shows a top view of a component of a substrate support in accordance with an embodiment and a component surrounding the substrate support in accordance with an embodiment.

FIG. 11 shows a top view of a component of a substrate support in accordance with another embodiment and a component surrounding the substrate support in accordance with another embodiment.

FIG. 12 shows a top view of a component of a substrate support in accordance with yet another embodiment and a component surrounding the substrate support in accordance with yet another embodiment.

FIG. 13 shows a top view of an etch rate pattern after partial etching of a substrate.

FIG. 14 shows a top view of an etch rate pattern after final etching of a substrate.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Precise azimuthal CD control on a substrate by small (e.g., <5° C.) corrections azimuthally to the substrate temperature can address CD uniformity which is sensitive to substrate temperature (e.g., as high as 1 nm/° C.). For example, even with an azimuthally symmetric etch chamber design, film thickness non-uniformity can result in azimuthal etch rate non-uniformity, as regions of substrate with thinner films undergo film clearing faster than other regions on the substrate. Small variabilities in hardware also contribute to azimuthal etch rate non-uniformity (e.g., <1%). Large applied DC magnetic fields (e.g., >20 Gauss), such as those used for plasma generation, can be a source of etch rate non-uniformity in plasma etching. Such a magnetic field induces a force, F, defined by F=E×B (where E is the electric field in the plasma and B is the magnetic field) on electrons in the plasma which results in azimuthal non-uniformity in the plasma during plasma etching, such non-uniformity in the plasma can lead to non-uniformity in the etch rate.

FIG. 1 shows a cross-sectional perspective of a substrate 70 and substrate support assembly 100 comprising a tunable ESC. The tunable ESC comprises a baseplate 10 with coolant fluid channels 20 disposed therethrough. A thermal insulating layer 30 is disposed on baseplate 10. A heating plate 40 is disposed on insulating layer 30 and comprises an array of discrete heating zones 50 distributed laterally across the substrate support and is operable to tune a spatial temperature profile for CD control. A ceramic plate 60 is disposed on heating plate 40. A substrate 70 is disposed over the ceramic plate 60 and is electrostatically clamped to the ESC by an electrostatic chucking electrode 61 embedded in the ceramic plate. It is noted that a substrate support 100 may comprise a standard, or non-tunable, ESC, instead of a tunable ESC. The substrate support assembly is adapted to support substrates of at least about 200 mm in diameter, or at least about 300 mm in diameter or at least about 450 mm in diameter. The materials of the components are not particularly limited. Baseplate 10 is preferably made from a suitable thermal conductor, such as aluminum or stainless steel. Ceramic plate 60 is preferably made from a suitable ceramic material, such as aluminum oxide (Ah03) or aluminum nitride (AlN). Thermal insulating layer 30 preferably comprises a silicone material, which adheres baseplate 10 to heating plate 40. An epoxy, silicone or metallurgical bond is preferably used to adhere heating plate 40 to ceramic plate 60.

Under operational conditions (e.g., plasma etching), DC magnetic fields used for plasma generation are a known source of etch rate non-uniformity. For example, a magnetic field parallel to the plane of substrate undergoing processing in the plasma volume is expected to induce non-uniformity in the azimuthal etch rate pattern with about 5% etch rate non-uniformity induced per Gauss of applied magnetic field. Thin film thickness variation and etch chamber hardware variation are also known to contribute to azimuthal etch rate non-uniformity.

The induced non-uniformity can be used to make adjustments to the azimuthal etch rate pattern using applied DC magnetic fields. These applied magnetic fields are relatively small (e.g., <20 Gauss or <10 Gauss, preferably ≤1 Gauss or ≤½ Gauss) and allow for localized corrections to the plasma processing such as etch rate to be made without significantly affecting other etch parameters (e.g. CD uniformity, substrate temperature). For example, the relatively small applied magnetic field also minimizes potential damage to circuits on a substrate being etched. Thus, when an azimuthal etch rate non-uniformity is detected in an etching process, such as those induced by film thickness variation, etch chamber hardware and the magnetic field of the plasma, a localized magnetic field above a substrate and generated from the substrate support can be used to make adjustments to an azimuthal etch rate pattern. Similar results can be obtained in other plasma processing such as plasma assisted deposition.

To apply such a localized magnetic field, at least one current carrying conductor (current loop) may be powered. FIG. 2 illustrates a current carrying conductor 150 embedded in a component of a substrate support assembly 100 (FIG. 2A). When DC current flows through the current carrying conductor 150, a magnetic field is generated predominantly in a direction perpendicular (FIG. 2B) to substrate support assembly 100 and substrate 70. Under operational conditions (e.g., plasma etching), the conductor 150 is operated independently of the other components of substrate support assembly 100, such as RF to the baseplate 10 and power to the heating plate 40 and voltage to the ESC. The conductor 150 is adapted to generate a DC magnetic field when DC power is supplied thereto by electrical leads running through the body of the component.

In order to generate small magnetic fields, a plurality of conductors 150 are laterally spaced across the substrate support and/or edge ring at locations suitable to generate applied magnetic fields effective to make corrections and/or adjustments to plasma processing such as an etch rate pattern. The conductors 150 may be located in a component such as an ESC ceramic, such as ceramic plate 60. The conductors 150 may be located in another component, such as baseplate 10. The conductors 150 may also be located in hardware adjacent the substrate support, such as an edge ring. Preferably, the current carrying conductors 150 are placed inside baseplate 10, such that any heat generated due to electrical current flow inside the conductors does not substantially alter the substrate temperature. If incorporated in baseplate 10, the conductors 150 are preferably wires with an electrically insulating sheath.

The current carrying conductor 150 may preferably comprise a wire, cable or conductive trace that is electrically isolated from its surroundings to ensure that the applied DC current only flows inside the conductor and not within the substrate support component in which it is embedded. Electrical isolation may be realized by providing a thin electrically insulating layer, or layers, surrounding current carrying conductor 150. For example, if current carrying conductor 150 is disposed in a component that is electrically conductive, a thin layer, or layers, of electrically insulating material or sheath is disposed around the conductor for electrical isolation. The electrically insulating material may comprise a Kapton film, an epoxy film, a silicone film and combinations thereof. If current carrying conductor 150 is disposed in a component that is electrically non-conductive, a thin layer, or layers, of electrically insulating material or sheath is not required for electrical isolation. The material of conductor 150 preferably comprises copper, but may be comprised of other materials with a suitable electrical conductivity.

The conductor 150 may be disposed within a component of a substrate support such that it forms a current loop 150. The current loop 150 may be formed into any desirable shape within the component and with reference to the plane of the upper surface of the substrate 70 and is preferably circular or semi-circular. Other shapes may be oval, semi-oval, square, rectangular, trapezoidal, triangular or other polygonal shape. If a wire is chosen for conductor 150 to be incorporated in ceramic plate 60, a wire may be placed at a desired location in a mold containing powder starting materials of the component. The molded component is then fired to form the component. If a conductive trace is chosen for conductor 150, a powder starting material of the trace may be formed into a pattern in a powder molding, with subsequent firing of the molding to form the component. If a conductive trace is chosen for conductor 150 and is to be placed on an outer surface of a component, a metal or other material may be plated on the component, with subsequent etching of the metal or other material to form the current loop on the component. If an individual wire is chosen as the conductor 150 and is to be formed on an upper surface of a component, a groove may be machined into the surface with dimensions suitable for receiving the wire and the insulated wire can be mounted in the groove with a suitable adhesive.

The current loop 150 can be supplied DC power by electrical leads connected thereto. FIG. 3 shows a perspective view of a substrate support assembly 100 comprising current loop 150 with leads 130 for power supply (up arrow) and power return (down arrow). The current loop 150 is disposed in or on baseplate 10. The leads are spaced a few mm apart such that the magnetic fields generated on the leads, and particularly those proximate the current loop 150, cancel each other out and do not interfere in the magnetic field over the substrate 70 being etched (FIG. 2A).

A current loop, or loops, may comprise a single turn. However, a current loop, or loops, comprising a plurality of turns to form a coil, or coil-like, structure are also contemplated. The coil, or coil-like, structure may reduce the DC current required for generating the applied magnetic field during an etching process. The embodiments of the current loop, or loops, are preferably disposed in planes parallel to the substrate. However, the current loop, or loops, may be disposed in planes that are not parallel to the substrate if such a disposition is desired.

The dimensions of current carrying conductor 150 are not particularly limited so long as the dimensions render its applied magnetic field effective to make corrections and/or adjustments to the plasma to achieve uniform processing such as an azimuthal etch rate pattern. The length of current carrying conductor 150 may be chosen such that the corresponding current loop 150 may be shaped into a desired form. For example, if a 300 mm diameter wafer is to be etched, each localized magnetic field can be generated by a single circular shaped current loop formed with a loop diameter between about 1-150 mm and preferably between about 1-75 mm. Depending on the shape of the current loop and the desired number of currently loops in the substrate support, the length of an individual current loop may be 5-1000 mm, e.g., 5-50 mm or 50-1000 mm, such as in the case of a component comprising up to two hundred current loops. The diameter of current carrying conductor 150 itself is also not particularly limited and may be any diameter or dimension that forms a suitable applied localized magnetic field. For example, if a 300 mm diameter wafer is to be etched, the current loop may be a wire with a diameter of between about 0.5 mm-10 mm and preferably between about 0.5 mm-5 mm. If a conductive trace is to be the current loop 150, the trace may be formed in a rectangular shape with a thickness of between about 0.5 mm-10 mm, preferably between about 0.5 mm-5 mm, and a width of between about 0.5 mm-10 mm, preferably between about 0.5 mm-5 mm. The direction of current flowing in the current loop is not particularly limited and may be either clockwise or counter-clockwise. Preferably, the current flowing in current loop 150 is adapted to be reversible to switch the direction of the current flow, and thus, switching the direction of the applied DC magnetic field, if desired.

For purposes of explanation, FIG. 2 shows an embodiment of a component of a substrate support assembly 100 comprising a single current loop 150. However, to provide localized magnetic fields it is desirable to have a plurality of current loops 150 in the substrate support. A plurality of current loops 150 allows for reduction of DC current required for a localized magnetic field strength over a substrate. An advantage of a plurality of current loops 150 is that each loop can be operated independently of one another such that each current loop may be supplied varying power levels and processing non-uniformity can be corrected and/or adjusted more efficiently. If each of the current loops 150 in the plurality of current loops is independently operable, further fine tuning capabilities are imparted to the applied magnetic field over the substrate. Preferably, as shown in FIG. 2C, the plurality of current loops 150 are connected to one or more DC power sources 152 controlled by a controller 154 such that the loops can be supplied power at the same or different times with the same or different power levels. Preferably, the DC power source, or sources, comprise a multiplexed powering scheme and can supply power to each current loop 150 such that each loop can be individually tuned by time-domain multiplexing. Preferably, the periphery of each current loop 150 in a plurality of current loops is laterally offset from the periphery of an adjacent current loop such that no overlap occurs. Preferably, the plurality of current loops 150 are disposed in a laterally symmetric or equidistant manner such that a plane that vertically intersects the center of the component where the loops are disposed produces substantial mirror images of each half of the component. The current loops 150 in the component are preferably arranged in a defined pattern, for example, a rectangular grid, a hexagonal grid, a polar array or any desired pattern.

FIG. 4 shows a preferred embodiment of a component of a substrate support assembly 100 wherein substrate support 100 comprises a plurality of current loops 150. FIG. 4 shows a preferred embodiment having two separate current loops 150 which are D-shaped and having their straight legs facing each other. The current loops 150 may be of the same size or may be of different sizes. Preferably, each of the current loops 150 extends less than about halfway around the support or edge ring. The current loops 150 are shown as being disposed towards a peripheral area of the substrate support component, but may also be disposed at any radial position desired. When the currents of these two loops are applied in the same direction (e.g., both clockwise or both counter-clockwise), a magnetic field similar to that shown in FIG. 2A is generated. When the currents of the two loops are applied in opposite directions (e.g., one clockwise and one counter-clockwise), certain portions of the applied magnetic field are cancelled over the center of the substrate.

FIG. 5 shows a preferred embodiment of a component of a substrate support assembly 100 wherein a substrate support 100 comprises multiple current loops 150. FIG. 5 shows a preferred embodiment with four separate current loops 150 which are each D-shaped and having their straight legs facing inward. Similar to those shown in FIG. 4, the current loops 150 are shown as being disposed towards a peripheral area of the substrate support component, but may also be disposed at any radial position desired. The four current loops 150 are capable of generating applied magnetic fields in various directions over the substrate depending on the direction of the current in each of the four loops 150, similar to the applied magnetic field generated by the two separate loops in FIG. 4.

FIG. 6 shows an embodiment of a component of a substrate support assembly 100 having circular current loops wherein controlling the direction of current in various current loops 150, more complex magnetic field patterns can be generated over the substrate. The embodiment of FIG. 6 comprises nine separate current loops 150, with eight outer current loops surrounding a center current loop. If desired, the total number of current loops 150 may be significantly more than nine, and can be as high as about two hundred. The more current loops 150, the more fine tuning capability imparted to the applied magnetic field over the substrate.

FIG. 7 shows an embodiment of a substrate support assembly 100 wherein a component adapted to surround a substrate support 100 comprises at least one current loop 150, and wherein substrate support 100 does not comprise a current loop. The generation of the magnetic field from the component compensates for non-uniformity at the outermost edge of substrate 70. FIG. 7 shows an embodiment wherein an edge ring 110 comprises two current loops 150 disposed in a plane substantially parallel to an upper surface of substrate 70. The current loops 150 are formed into a block semi-circular shape that substantially surround substrate support 100 and are disposed on opposite sides of edge ring 110. The loops are independently operated with respect to each other such that two magnetic fields can be generated. The major legs of the current loops can be on the same or different planes. FIG. 8 shows a perspective view of current loop 150 disposed in edge ring 110. The loop includes major legs which are vertically offset with electrical leads 130 for power supply (up arrow) and power return (down arrow). The leads are spaced a few mm apart such that the magnetic fields generated on the leads, and particularly those proximate the current loop 150, cancel each other out and do not interfere in the magnetic field over the substrate 70 being etched (FIG. 2A). If desired, edge ring 110 may comprise more than two current loops 150. FIG. 9 shows an embodiment wherein edge ring 110 comprises four current loops 150 and wherein substrate support 100 does not comprise any current loops. Each of the four current loops 150 are arranged diametrically opposite to another one of the loops 150.

FIG. 10 shows an embodiment of a component of a substrate support assembly 100 wherein both substrate support 100 and a component 110 surrounding the substrate support comprise at least one current loop 150. Adding at least one current loop 150 to such hardware, such as edge ring 110 surrounding the substrate support 100, extends the influence of the applied magnetic field over the substrate to the outermost edge of substrate 70. In the embodiment of FIG. 10, the substrate support 100 and edge ring 110 each comprise two current loops 150. The current loops incorporated in the substrate support are D-shaped with the straight legs facing each other. The current loops incorporated in the edge ring are offset 90° with respect to the current loops of the substrate support. The current loops 150 in the substrate support 100 and edge ring 110 may or may not be planar with respect to each other or with respect to a substrate surface. The current loops 150 in the edge ring 110 preferably extend around a substantial portion of its circumference.

The number of current loops 150 that the substrate support assembly 100 comprise may be greater than two, such as that shown in FIG. 11, wherein both substrate support 100 and edge ring 110 each comprise four current loops 150. FIG. 12 shows an embodiment of a substrate support assembly 100 wherein the support comprises nine current loops 150 and edge ring 110 comprises twelve current loops 150. The current loops 150 comprised in the substrate support or edge ring are laterally distributed in a symmetric manner.

The current loops can be incorporated in any type of substrate support which may or may not include an electrostatic clamping arrangement, heating arrangement and/or temperature controlled baseplate. In a preferred method of controlling and/or adjusting an etch rate pattern using a substrate support incorporating current loops, a substrate is supported on a substrate support comprising a baseplate, a thermal insulating layer disposed over the baseplate, a heating plate disposed over the thermal insulating layer, a ceramic plate disposed over the a thermal insulating layer; and current loops; etching a substrate disposed on the substrate support; detecting an etch rate non-uniformity, such as an azimuthal etch rate non-uniformity, after etching has been initiated; and providing one or more of the current loops with DC power to generate localized DC magnetic fields that correct and/or adjust the etch rate non-uniformity.

An azimuthal etch rate non-uniformity may be detected as follows. A substrate comprising a thin film, such as a polysilicon thin film in the case of semiconductor substrate, to be processed is inspected to determine the thickness of the thin film at various locations across the substrate using standard interferometry techniques. The substrate is then plasma etched, or partially etched. After etching, or partial etching, the thickness of the thin film is measured again using standard interferometry techniques. The difference between the two thin film thickness measurements is determined by an appropriate algorithm, which also is able to generate an etch pattern on the substrate surface. From an etch rate pattern, a mean depth of the film thickness left on the substrate is determined, along with other parameters, such as the standard deviation and global maximum and minimum depths. These parameters are used to determine where selective application of a magnetic field can be applied to correct and/or adjust an azimuthal etch rate non-uniformity during subsequent etching of a batch of wafers undergoing the same etch process.

Alternatively, incoming wafer thickness of a substrate can be measured, the B-field pattern to provide uniform etching can be determined, and etching of a batch of substrates can be carried out. In another method, a substrate can be etched, an azimuthal pattern for etching can be determined, the magnetic field compensation is determined and further substrates are etched while applying the magnetic field compensation. The etch rate or other parameters could be monitored during plasma etching and the current loops could be powered to compensate for local etch rate variation during the plasma etch process.

Example 1

A silicon wafer with a 1 μm thick silicon oxide film on its surface to be etched to a depth of about 400 nm is surrounded by an edge ring with two current loops, similar to the configuration of FIG. 7, wherein the supply trace and return trace are non-planar. Etching can be carried out using a fluorocarbon etching gas. The substrate is loaded into a plasma etch vacuum chamber and is partially etched to a depth of about 200 nm and then removed from the chamber. Interferometric techniques are used to determine the etch rate non-uniformity by measuring the film thickness profile over the substrate before and after partial etching. From these measurements, an algorithm is used to generate the etch rate pattern. After analysis of the pattern, parameters used to determine corrections and/or adjustments to be carried out to the azimuthal etch rate non-uniformity are determined. The partial etch is determined to result in average depth in the film of 192.4 nm, with a three-sigma standard deviation of 19.2 nm (10%). The difference between a global maximum and minimum is 31.9 nm (16.6%). Analysis of the etch rate pattern is shown in FIG. 13. Areas 190 (in black) on substrate 70 are shown to be etched with a faster etch rate than areas 180 (in gray).

Etching the remaining portions of the film on substrate 70 is then carried out. During the subsequent etching, DC power is supplied to the current loops 150 disposed in edge ring 110. DC power is supplied such that an 3 Gauss magnetic field is generated by the loops 150. After completion of etching, the etch rate pattern is determined, as described above. This etch results in an average of 189.5 nm of film thickness removed, with a three-sigma standard deviation of 13.9 nm (7.3%). The difference between a global maximum and minimum is 25.2 nm (13.3%). Analysis of the etch rate pattern is shown in FIG. 14. Areas 190 (in gray) on substrate 70 are shown to be etched with a slower etch rate than areas 180 (in black).

Thus, etching a substrate in the presence of an applied DC magnetic field can compensate for etch rate non-uniformity and thus provide a more uniform etch rate. With an applied magnetic field of about 3 Gauss generated from current loops in an edge ring, azimuthal etch rate non-uniformity can be decreased by about 3.3.% (range after partial etch—range after final etch), with a decrease in the three-sigma standard deviation of about 2.7% (deviation after partial etch —deviation after final etch). Furthermore, application of an 3 Gauss magnetic field shows that areas etched at a faster etch rate in the partial etch can be etched at a slower etch rate in the final etch step, thus, correcting for an azimuthal etch rate non-uniformity. Similarly, application of an 3 Gauss magnetic field shows that the areas that are etched at a slower etch rate in the partial etch can be etched at a faster etch rate in the final etch step, thus, correcting for an azimuthal etch rate non-uniformity.

Example 2

In a process scheme to compensate for etch rate variation:

a. a wafer is partially etched and the etch rate non-uniformity is measured;

b. apply a magnetic field pattern to the plasma above a wafer (based on historical knowledge);

c. etch another wafer, determine etch pattern sensitivity to the applied magnetic field pattern since the applied field is known; and

d. optionally repeat steps a-c to determine an optimal magnetic field pattern.

Example 3

In a process scheme to compensate for incoming wafer thickness variation:

a. measure incoming wafer thickness variation;

b. apply a magnetic field pattern (based on historical knowledge);

c. etch a wafer, determine etch pattern sensitivity to the applied magnetic field pattern since the applied field is known; and

d. optionally repeat steps a-c and adjust the applied magnetic field pattern if necessary.

All of the above-mentioned references are herein incorporated by reference in their entirety to the same extent as if each individual reference was specifically and individually indicated to be incorporated herein by reference in its entirety.

While the invention has been described with reference to preferred embodiments, it is to be understood that variations and modifications may be resorted to as will be apparent to those skilled in the art. Such variations and modifications are to be considered within the purview and scope of the invention as defined by the claims appended hereto.

Claims

1. A component of a substrate support assembly useful for supporting individual semiconductor substrates undergoing plasma processing, the component comprising:

an electrostatic chuck for supporting a semiconductor substrate during plasma processing thereof or an edge ring which surrounds the semiconductor substrate, wherein the electrostatic chuck includes an embedded electrode receiving a first voltage to electrostatically attract the semiconductor substrate to the substrate support assembly; and
a plurality of current loops incorporated in the electrostatic chuck or the edge ring, the plurality of current loops being laterally spaced apart and extending less than halfway around the electrostatic chuck or edge ring, each of the plurality of current loops being a wire formed into a loop;
one or more DC power sources electrically connected to the plurality of current loops; and
a controller configured to:
supply the first voltage to the embedded electrode;
supply a DC current to the plurality of current loops from the one or more DC power sources, the DC current directly supplied to the plurality of current loops being separate from and in addition to the first voltage supplied to the embedded electrode; and
control the one or more DC power sources such that each of the plurality of current loops is independently operable and generates a localized DC magnetic field above the semiconductor substrate supported on the electrostatic chuck when the DC current is applied to a current loop of the plurality of current loops during plasma processing of the semiconductor substrate to adjust or correct the plasma processing of the semiconductor substrate
wherein the localized DC magnetic field generated by the plurality of current loops does not generate plasma.

2. The component of claim 1, wherein the electrostatic chuck includes a baseplate, a thermal insulating layer above the baseplate, and a ceramic plate with the embedded electrode above the thermal insulating layer; and the plurality of current loops are embedded in the baseplate or the ceramic plate such that the plurality of current loops lie substantially in a plane parallel to an upper surface of the semiconductor substrate.

3. The component of claim 1, wherein the plurality of current loops are embedded in the edge ring such that the plurality of current loops lie substantially in a plane parallel to an upper surface of the semiconductor substrate.

4. The component of claim 1, wherein the plurality of current loops includes up to 200 current loops that have the same size and a circular shape and that are embedded in the electrostatic chuck or the edge ring.

5. The component of claim 1, wherein each of the plurality of current loops has a circular, semi-circular, oval, semi-oval, square, rectangular, trapezoidal, triangular or polygonal shape.

6. The component of claim 1, wherein the wire has a diameter of between about 0.5-10 mm.

7. The component of claim 1, wherein a periphery of each current loop of the plurality of current loops is laterally offset from a periphery of an adjacent current loop of the plurality of current loops.

8. A plasma processing chamber incorporating the component of claim 1, wherein the electrostatic chuck includes a heater layer having a plurality of heaters laterally distributed across the electrostatic chuck and operable to tune a spatial temperature profile for critical dimension (CD) control, the plurality of current loops including at least 9 current loops distributed laterally across the electrostatic chuck and operable to compensate for local non-uniformity in processing on the semiconductor substrate.

9. The plasma processing chamber of claim 8, wherein the plasma processing chamber is a plasma etching chamber.

10. The plasma processing chamber of claim 8, wherein the controller is configured to control the one or more DC power sources such that the one or more DC power sources supply the DC current to the plurality of current loops at the same time or different times with the same or different levels of the DC current, and wherein the DC current flows in the plurality of current loops in the same direction or different directions.

11. A method of controlling and/or adjusting a magnetic field pattern during plasma processing of the semiconductor substrate undergoing processing in the plasma processing chamber of claim 8, comprising:

a) supporting the semiconductor substrate on the electrostatic chuck;
b) plasma processing the semiconductor substrate; and
c) supplying at least one of the plurality of current loops with the DC current to generate the localized DC magnetic field in a region above the semiconductor substrate so as to compensate for local non-uniformity in processing.

12. The method of claim 11, further comprising supplying the plurality of current loops with different amounts of the DC current, with the DC current travelling in a clockwise direction in each of the plurality of current loops.

13. The method of claim 11, further comprising supplying the plurality of current loops with different amounts of the DC current, with the DC current travelling in different directions in some of the plurality of current loops.

14. The method of claim 11, wherein each of the plurality of current loops generates the localized DC magnetic field above the semiconductor substrate with a field strength of less than 1 Gauss.

15. The method of claim 14, wherein the field strength is less than 20 Gauss or less than 0.5 Gauss.

16. The method of claim 11, wherein the plurality of current loops includes at least two current loops, and wherein the electrostatic chuck is surrounded by an edge ring having the at least two current loops, with each of the at least two current loops arranged on an opposite side of the edge ring.

17. The method of claim 16, wherein the plurality of current loops includes at least four current loops; wherein the edge ring has the at least four current loops, with each of the at least four current loops arranged diametrically opposite to another one of the at least four current loops; and wherein each of the at least four current loops has a circular, semi-circular, oval, semi-oval, square, rectangular, trapezoidal, triangular or polygonal shape.

18. The method of claim 11, wherein the plasma processing is plasma etching and further comprising, after steps a) and b) and prior to step c):

removing the semiconductor substrate from the plasma processing chamber;
detecting an etch-rate non-uniformity in an etch-rate pattern on the semiconductor substrate; and
modifying step c) so as to compensate for film thickness induced etch-rate non-uniformity, etch chamber induced etch-rate non-uniformity or plasma induced etch-rate non-uniformity.

19. The method of claim 11, wherein the DC current is supplied from the one or more DC power sources comprising a multiplexed power scheme.

20. The method of claim 11, wherein the electrostatic chuck is adapted to support the semiconductor substrate having a diameter of at least about 200 mm, at least about 300 mm or at least about 450 mm.

Referenced Cited
U.S. Patent Documents
3440883 April 1969 Lightner
4099228 July 4, 1978 Cohn
4692836 September 8, 1987 Suzuki
5059770 October 22, 1991 Mahawili
5255520 October 26, 1993 O'Geary et al.
5414245 May 9, 1995 Hackleman
5436528 July 25, 1995 Paranjpe
5504471 April 2, 1996 Lund
5515683 May 14, 1996 Kessler
5536918 July 16, 1996 Ohkase et al.
5635093 June 3, 1997 Arena et al.
5665166 September 9, 1997 Deguchi et al.
5667622 September 16, 1997 Hasegawa et al.
5740016 April 14, 1998 Dhindsa
5745332 April 28, 1998 Burkhart
5802856 September 8, 1998 Schaper et al.
5851298 December 22, 1998 Ishii
5880923 March 9, 1999 Hausmann
5886866 March 23, 1999 Hausmann
5994675 November 30, 1999 Bethune et al.
6060697 May 9, 2000 Morita et al.
6091060 July 18, 2000 Getchel et al.
6095084 August 1, 2000 Shamouilian
6100506 August 8, 2000 Colelli, Jr. et al.
6175175 January 16, 2001 Hull
6216632 April 17, 2001 Wickramanayaka
6222161 April 24, 2001 Shirakawa et al.
6271459 August 7, 2001 Yoo
6332710 December 25, 2001 Aslan et al.
6339997 January 22, 2002 Nakagawa
6342997 January 29, 2002 Khadkikar et al.
6353209 March 5, 2002 Schaper et al.
6403403 June 11, 2002 Mayer et al.
6475336 November 5, 2002 Hubacek
6483690 November 19, 2002 Nakajima et al.
6495963 December 17, 2002 Bennett
6512207 January 28, 2003 Dress et al.
6523493 February 25, 2003 Brcka
6566632 May 20, 2003 Katata et al.
6612673 September 2, 2003 Giere et al.
6664515 December 16, 2003 Natsuhara et al.
6739138 May 25, 2004 Saunders et al.
6740853 May 25, 2004 Johnson et al.
6741446 May 25, 2004 Ennis
6746616 June 8, 2004 Fulford et al.
6795292 September 21, 2004 Grimard et al.
6815365 November 9, 2004 Masuda et al.
6825617 November 30, 2004 Kanno et al.
6835290 December 28, 2004 Reiter et al.
6847014 January 25, 2005 Benjamin et al.
6870728 March 22, 2005 Burket et al.
6886347 May 3, 2005 Hudson et al.
6921724 July 26, 2005 Kamp et al.
6979805 December 27, 2005 Arthur et al.
6985000 January 10, 2006 Feder et al.
6989210 January 24, 2006 Gore
7075031 July 11, 2006 Strang et al.
7141763 November 28, 2006 Moroz
7173222 February 6, 2007 Cox et al.
7175714 February 13, 2007 Ootsuka et al.
7206184 April 17, 2007 Ennis
7230204 June 12, 2007 Mitrovic et al.
7250309 July 31, 2007 Mak et al.
7268322 September 11, 2007 Kuibira et al.
7274004 September 25, 2007 Benjamin et al.
7275309 October 2, 2007 Matsuda et al.
7279661 October 9, 2007 Okajima et al.
7297894 November 20, 2007 Tsukamoto
7311782 December 25, 2007 Strang et al.
7372001 May 13, 2008 Tachikawa et al.
7396431 July 8, 2008 Chen et al.
7415312 August 19, 2008 Barnett, Jr. et al.
7430984 October 7, 2008 Hanawa et al.
7475551 January 13, 2009 Ghoshal
7480129 January 20, 2009 Brown et al.
7504006 March 17, 2009 Gopalraja et al.
7512359 March 31, 2009 Sugiyama
7718932 May 18, 2010 Steger
7782583 August 24, 2010 Moon
7893387 February 22, 2011 Ohata
7940064 May 10, 2011 Segawa et al.
7952049 May 31, 2011 Tsukamoto
7968825 June 28, 2011 Jyousaka et al.
8057602 November 15, 2011 Koelmel et al.
8136820 March 20, 2012 Morioka et al.
8168050 May 1, 2012 Lu
8207476 June 26, 2012 Tsukamoto et al.
8222574 July 17, 2012 Sorabji et al.
8295026 October 23, 2012 Matsuyama
8461674 June 11, 2013 Gaff et al.
8536492 September 17, 2013 Ramamurthy et al.
8546732 October 1, 2013 Singh
8624168 January 7, 2014 Gaff et al.
8637794 January 28, 2014 Singh et al.
8642480 February 4, 2014 Gaff et al.
8791392 July 29, 2014 Singh
8809747 August 19, 2014 Pease et al.
20020043528 April 18, 2002 Ito
20030150712 August 14, 2003 Reiter et al.
20040110388 June 10, 2004 Yan et al.
20050016465 January 27, 2005 Ramaswamy
20050120956 June 9, 2005 Suzuki
20050215073 September 29, 2005 Nakamura et al.
20060191637 August 31, 2006 Zajac et al.
20060226123 October 12, 2006 Birang
20060229854 October 12, 2006 Grichnik et al.
20070000918 January 4, 2007 Steinhauser et al.
20070125762 June 7, 2007 Cui et al.
20080029195 February 7, 2008 Lu
20080049374 February 28, 2008 Morioka et al.
20080202924 August 28, 2008 Bluck et al.
20090000738 January 1, 2009 Benjamin
20090173445 July 9, 2009 Yeom
20090183677 July 23, 2009 Tian et al.
20090215201 August 27, 2009 Benjamin et al.
20100078424 April 1, 2010 Tsukamoto et al.
20100116788 May 13, 2010 Singh et al.
20100163546 July 1, 2010 Nanno et al.
20100257871 October 14, 2010 Venkatasubramanian et al.
20100283565 November 11, 2010 Blakes
20110005682 January 13, 2011 Savas et al.
20110033175 February 10, 2011 Kasai et al.
20110092072 April 21, 2011 Singh
20110095689 April 28, 2011 Gilbert
20110108706 May 12, 2011 Koyama
20110143462 June 16, 2011 Gaff et al.
20120031889 February 9, 2012 Komatsu
20120097661 April 26, 2012 Singh
20120115254 May 10, 2012 Singh
20130003250 January 3, 2013 Morimoto et al.
20130072035 March 21, 2013 Gaff et al.
20130220989 August 29, 2013 Pease et al.
20140048529 February 20, 2014 Pease et al.
Foreign Patent Documents
601918 January 1985 JP
621176 January 1987 JP
06010391 March 1994 JP
H06-077146 March 1994 JP
H09-087839 March 1997 JP
H11-283926 October 1999 JP
2002-313535 October 2002 JP
2004152913 May 2004 JP
2005123286 May 2005 JP
2005294237 October 2005 JP
2006-509365 March 2006 JP
2007081160 March 2007 JP
2007082374 March 2007 JP
2009267256 November 2009 JP
2010153730 July 2010 JP
2010-225941 October 2010 JP
2011-018684 January 2011 JP
201998028601 August 1998 KR
1020050053464 June 2005 KR
20050121913 December 2005 KR
1020060067552 June 2006 KR
20080058109 June 2008 KR
Other references
  • International Preliminary Report on Patentability dated Mar. 18, 2014 for PCT/US2012/053386.
  • Ayars, Eric, “Bandgap in a Semiconductor Diode”, Advanced and Intermediate Instructional Labs Workshop, AAPT Summer Meeting, California State university, Chicago, Jul. 20, 2008 http://phys.csuchico.edu/-eayars/publications/bandgap.pdf.
  • International Search Report and Written Opinion dated Nov. 16, 2012 for PCT/US2012/053386.
  • Commonly-Owned Utility U.S. Appl. No. 12/910,347, filed Oct. 22, 2010.
  • Commonly-Owned Utility U.S. Appl. No. 12/943,492, filed Nov. 10, 2010.
  • Commonly-Owned Utility U.S. Appl. No. 13/237,444, filed Sep. 20, 2011.
  • Commonly-Owned Utility U.S. Appl. No. 13/238,396, filed Sep. 21, 2011.
  • Taiwanese First Office Action dated Mar. 16, 2016 by Taiwanese Intellectual Property Office in Taiwanese Application No. 101132350 (with English language translation).
  • Office Action (Notification of the Final Office Action) dated Apr. 26, 2016, by the Korean Patent Office in corresponding Korean Patent Application No. 10-2013-7012033, and a Partial English Translation of the Office Action. (5 pages).
  • Office Action (Notice of Reasons for Rejection) dated Aug. 9, 2016, by the Japanese Patent Office in corresponding Japanese Patent Application No. 2014-530690, and an English Translation of the Office Action. (13 pages).
  • Notification of Transmittal of the International Search Report (Forms PCT/ISA/220 and PCT/ISA/210) and the Written Opinion of the International Searching Authority (Form PCT/ISA/237) dated Oct. 23, 2012, in the International Application No. PCT/US2012/051029. (12 pages).
  • Notification of Transmittal of the International Search Report (Forms PCT/ISA/220 and PCT/ISA/210) and the Written Opinion of the International Searching Authority (Form PCT/ISA/237) dated Apr. 4, 2013, in the International Application No. PCT/US2013/023823. (9 pages).
  • Notification Concerning Transmittal of International Preliminary Report on Patentability (Forms PCT/IB/326 and PCT/IB/373) and the Written Opinion of the International Searching Authority (Form PCT/ISA/237) dated Sep. 12, 2014, by the International Bureau of WIPO in the International Application No. PCT/US2013/023823. (7 pages).
Patent History
Patent number: 10388493
Type: Grant
Filed: Sep 16, 2011
Date of Patent: Aug 20, 2019
Patent Publication Number: 20130072025
Assignee: Lam Research Corporation (Fremont, CA)
Inventors: Harmeet Singh (Fremont, CA), Keith Gaff (Fremont, CA), Brett Richardson (San Ramon, CA), Sung Lee (Pleasanton, CA)
Primary Examiner: Benjamin Kendall
Assistant Examiner: Mirza Israr Javed
Application Number: 13/234,473
Classifications
Current U.S. Class: With Magnetic Or Electrostatic Means (279/128)
International Classification: H01F 7/20 (20060101); H01J 37/32 (20060101); H01L 21/67 (20060101); H01L 21/311 (20060101);